Audited 31 Jul 2026·Last updated 28 Oct 2026·5 citations·Tier 1·0 uses

Cv Liquid Flow Calculator

Predict liquid flow through a valve in US gpm from its Cv, the pressure drop across it in psi and the liquid's specific gravity, using Q = Cv × √(ΔP ÷ SG).

Cv Liquid Flow Calculator

psi
Liquid flow rate
20
Predicted liquid flow through the valve in US gallons per minute, from Q = Cv × √(ΔP ÷ SG).
Model scope
US Cv convention for fully turbulent, nonflashing, noncavitating liquid flow with no attached-fitting correction; it does not size gas or steam, select a valve, establish allowable pressure drop, or apply viscosity, choking, piping-geometry, noise, erosion, or safety corrections.

Background.

Every control valve, ball valve and solenoid valve sold for liquid service has a flow coefficient, Cv, on its data sheet. It is the valve's capacity reduced to one number: the US gallons per minute of 60 °F water that pass through it with a pressure drop of 1 psi across it. A valve with a Cv of 10 passes 10 gpm of water at a 1 psi drop; one with a Cv of 100 passes ten times as much under the same conditions.

Real systems rarely run at exactly 1 psi, and they seldom carry plain water, so the coefficient has to be scaled. Flow through a restriction rises with the square root of the pressure drop and falls with the square root of the liquid's specific gravity: Q = Cv × √(ΔP ÷ SG). The square root is what catches people out. Quadrupling the pressure drop only doubles the flow, so a valve that is a little too small cannot be rescued by pushing much more pressure through it.

This is the basic US-unit liquid sizing relation found in control-valve handbooks and the ISA-75.01.01 standard, and it holds while flow through the valve is fully turbulent and stays liquid. It breaks down when the pressure inside the valve falls low enough for the liquid to start boiling: the flow cavitates or flashes and eventually chokes, and raising the pressure drop further adds noise and damage but no more flow. Viscous liquids, reducers fitted directly to the valve body, and gases or steam all need corrections or different equations that are not applied here.

Within those limits it is the quickest way to check whether an installed valve can pass the flow you need, or how much flow you lose when the supply pressure drops.

What is cv liquid flow calculator?

The result is the volumetric flow rate of a liquid through a valve, in US gallons per minute, predicted from the valve's flow coefficient Cv, the pressure difference between its inlet and outlet in psi, and the liquid's specific gravity — its density relative to water, so water is 1. Because Cv is defined with water at 60 °F and a 1 psi drop, water at a 1 psi drop returns exactly the Cv value.

Specific gravity belongs at the flowing temperature. Water at 80 °C has a specific gravity of about 0.97, which raises the predicted flow by only about 1.4%, so temperature seldom matters for water; it matters more for light hydrocarbons, whose density shifts faster as they warm. Rough values are 0.84 for diesel, 1.025 for seawater and above 1 for brines and glycol mixtures. Pipe size, by contrast, says little about capacity: a needle valve and a full-port ball valve with the same 1-inch connections can differ in Cv many times over, so it is the coefficient, not the connection size, that should be compared when choosing between valves.

How to use this calculator.

  1. Enter the Valve flow coefficient Cv from the manufacturer's data sheet, for the opening you care about. The rated figure usually describes a fully open valve; a throttled control valve has a smaller effective Cv.
  2. Enter the Pressure drop in psi across the valve itself — inlet pressure minus outlet pressure at the valve — not across the whole pipe run. To convert from bar, multiply by 14.504.
  3. Enter the Liquid specific gravity at the flowing temperature: 1 for water, below 1 for lighter liquids such as most oils and fuels, above 1 for brines and other dense fluids.
  4. Read the flow in US gallons per minute (multiply by 3.785 for litres per minute) and check the model-scope note: if the valve may be cavitating or the liquid is thick, real flow will be lower than shown.

The formula.

Q(gpm) = Cv sqrt(DeltaP(psi) / SG)

Q = Cv × √(ΔP ÷ SG), with Q in US gallons per minute, ΔP in pounds per square inch and SG dimensionless. There is no hidden constant because Cv is defined in exactly those units: at ΔP = 1 psi and SG = 1 the square root is 1 and Q equals Cv. Flow is directly proportional to Cv but depends on the square root of the other two terms, so doubling the pressure drop raises flow by only √2, about 41%, and a liquid 20% denser than water flows about 8.7% more slowly. Rearranged, the same relation sizes a valve: Cv = Q × √(SG ÷ ΔP). The metric counterpart, Kv, is defined in cubic metres per hour of water at a 1 bar drop, and Cv ≈ 1.156 × Kv.

The square root comes from an energy balance across the valve's narrowest passage. The pressure difference accelerates the liquid and most of it is lost to turbulence downstream, so ΔP = K × ρv² ÷ 2 for a loss coefficient K; solving for velocity and multiplying by the flow area gives Q proportional to A × √(ΔP ÷ (K × ρ)). Cv bundles the area, the loss coefficient and the unit conversions into one measured number, which is why it converts to a resistance coefficient for pipe-network work: for a valve of inside diameter d in inches, Cv = 29.9 × d² ÷ √K.

The same derivation marks the limits. It assumes fully turbulent flow, so that K, and therefore Cv, does not change with flow rate. It also assumes the liquid stays liquid. The ISA sizing standard caps the useful drop at FL² × (P1 − FF × Pv), where FL is the valve's liquid pressure-recovery factor from the manufacturer, P1 the absolute inlet pressure, Pv the vapour pressure of the liquid and FF a factor close to 0.96 for water at ordinary temperatures. For room-temperature water at 100 psia and a valve with FL = 0.9, the cap is about 80.72 psi; beyond it flow is choked. High-recovery designs such as ball and butterfly valves have lower FL values than globe valves and reach the cap at smaller drops.

A worked example.

Example

A valve with a Cv of 10 passes water, specific gravity 1, with 4 psi measured between its inlet and outlet. Divide the pressure drop by the specific gravity: 4 ÷ 1 = 4. Take the square root: √4 = 2. Multiply by the coefficient: 10 × 2 = 20 US gpm, about 75.7 litres per minute. Because of the square root, quadrupling the drop to 16 psi only doubles the flow, to 40 gpm, while doubling it to 8 psi gives 28.28 gpm. Pass a brine with specific gravity 1.2 through the same valve at the original 4 psi and the flow falls to 18.26 gpm. Run backwards, the same arithmetic diagnoses a valve. If a flowmeter shows only 12 gpm of water with 4 psi measured across this valve, its effective coefficient is 12 ÷ √(4 ÷ 1) = 6, well short of the rated 10: the valve is not fully open, its trim is fouled, or the gauges are reading a drop that includes pipe and fittings as well as the valve.

liquid Specific Gravity1
pressure Drop Psi4
valve Cv10

Frequently asked questions.

What exactly does a Cv of 1 mean?
A valve with a Cv of 1 passes one US gallon per minute of 60 °F water when the pressure on its inlet side is 1 psi higher than on its outlet side. The coefficient is a capacity rating: under identical conditions, a valve with twice the Cv passes twice the flow.
How do I convert between Cv and Kv?
Kv is the metric equivalent, in cubic metres per hour of water at a 1 bar drop. Cv ≈ 1.156 × Kv and Kv ≈ 0.865 × Cv. A Cv of 10 is a Kv of about 8.65, which at 4 psi (0.276 bar) gives about 4.54 m³/h, the same 75.7 litres per minute as the US-unit result.
Why doesn't doubling the pressure drop double the flow?
The pressure difference is spent accelerating the liquid through the valve's narrowest passage, and the energy needed rises with the square of velocity. Flow is therefore proportional to the square root of the pressure drop: twice the drop gives about 1.41 times the flow, and four times the drop gives double.
What is choked flow, and how can I tell if my valve is cavitating?
If the pressure at the narrowest point inside the valve falls below the liquid's vapour pressure, vapour bubbles form and then collapse downstream. Signs are a gravelly noise, vibration and pitted trim. Once flow chokes, raising the pressure drop no longer increases flow, so this equation will overpredict it. Flashing is the related case in which the outlet pressure itself stays below the vapour pressure, so the bubbles never collapse and a vapour–liquid mixture leaves the valve, eroding the trim instead of pitting it.
How do I work out the Cv a valve needs?
Rearrange the equation: Cv = Q × √(SG ÷ ΔP). Passing 50 gpm of water with 9 psi available across the valve needs a Cv of 50 × √(1 ÷ 9), about 16.67. For control valves, choose one whose required Cv falls well inside its travel rather than right at full open, so it can still regulate.
Can I use this for air, gas or steam?
No. Gases and steam are compressible, so their density changes as they pass through the valve, and sizing them needs separate equations with an expansion factor and inlet pressure and temperature. Applying the liquid formula to a gas gives a meaningless answer.
How do I combine the Cv of two valves in series or in parallel?
In parallel both valves see the same pressure drop and their flows add, so the coefficients simply add: a Cv 10 and a Cv 20 side by side act as Cv 30. In series the same flow passes through both and the drops add, so 1/Cv² = 1/Cv₁² + 1/Cv₂². The same pair in series acts as about Cv 8.94, passing 17.89 gpm of water at 4 psi, and the smaller valve takes 3.2 psi of that drop. The rule assumes each valve sees settled flow, so treat it as an estimate for valves bolted right next to each other.
My control valve is only partly open. What Cv should I enter?
The Cv at that opening, taken from the manufacturer's table of Cv against travel; it is usually well below the rated full-open figure. How far below depends on the trim. A linear trim gives roughly half its rated Cv at half travel. An ideal equal-percentage trim with a rangeability of 50 gives 50^(x − 1) of it, where x is the fraction open: about 14% at half travel, so a valve rated Cv 10 behaves like Cv 1.41 and passes only about 2.83 gpm of water at 4 psi.
Why did fitting a bigger valve barely raise the flow in my line?
Because the valve shares a fixed pressure budget with the pipe. Suppose a pump leaves 50 psi for pipe and valve together, and the pipe alone loses 20 psi at 20 gpm, its loss rising with the square of flow. With a Cv 10 valve the line settles at about 28.87 gpm, with 8.33 psi across the valve and 41.67 psi lost in the pipe. A Cv 20 valve lifts the flow only to about 30.86 gpm, because the pipe was the main restriction. The equation is right for whatever drop the valve actually sees, but it cannot predict that drop on its own.
Does a thick liquid such as heavy oil or syrup flow as predicted?
Often not. Cv is measured with water in turbulent flow, and a viscous liquid moving slowly through a small valve can fall into laminar or transitional flow, where friction takes a larger share of the pressure drop and the valve passes less than the equation says. The ISA standard handles this with a Reynolds-number factor, FR, that scales the coefficient down; it is not applied here, so for viscous service the result is an upper bound until the manufacturer's viscosity correction is applied.

How this page was produced

Published by
Quanta Calculator
Primary sources
5 cited below
Method
Q(gpm) = Cv sqrt(DeltaP(psi) / SG)
Published
Last verified

Built with AI assistance and verified by automated tests against the cited sources — every worked example on this page is computed by the same code that runs the calculator. How we build and check calculators.

In this category

Embed

Quanta Pro

Paid features are coming later.

  • All 1560 calculators remain free
  • No billing is enabled
Coming soon